The High-Power-Target System of a Muon Collider or Neutrino Factory - PowerPoint PPT Presentation

The High-Power-Target System of a Muon Collider or Neutrino Factory K. McDonald Princeton U. (March 5, 2012) Muon Accelerator Program Winter Meeting SLAC KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 1

The Target is the Interface between a Proton Driver and  or  Beams A Muon Collider is an energy-frontier particle-physics facility (that also produces lots of high-energy  ’s). Higher mass of muon  Better defined initial state than e + e - at high energy. A muon lives  1000 turns. Need lots of muons to have enough luminosity for physics. Need a production target that can survive multmegawatt proton beams. KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 2

Target and Capture Topology: Solenoid Desire  10 14  /s from  10 15 p /s (  4 MW proton beam) Superconducting magnets R.B. Palmer ( BNL , 1994) proposed a Present Target Concept: 20-T solenoidal capture system. Tungsten beads, He gas cooled Low-energy  's collected from side of long, thin cylindrical target. Be window Proton beam and Mercury jet Solenoid coils can be some distance from proton beam.   10-year life against radiation damage at 4 MW. Liquid mercury jet target replaced Mercury collection pool every pulse. With splash mitigator Resistive magnets Proton beam readily tilted with respect to magnetic axis. Shielding of the superconducting magnets from radiation is a major issue.  Beam dump (mercury pool) out of Magnet stored energy ~ 3 GJ! the way of secondary  's and  's. 5-T copper magnet insert; 15-T Nb 3 Sn coil + 5-T NbTi outsert. Desirable to replace the copper magnet by a 20-T HTC insert. KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 3

High Levels of Energy Deposition in the Target System Power deposition in the superconducting magnets and the He-gas-cooled tungsten shield inside them, according to a FLUKA simulation. Approximately 2.4 MW must be dissipated in the shield. Some 800 kW flows out of the target system into the downstream beam-transport elements. Total energy deposition in the target magnet string is ~ 1 kW @ 4k. Peak energy deposition is about 0.03 mW/g. KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 4

Large Cable-in-Conduit Superconducting Magnets The high heat load of the target magnet requires Nb 3 Sn cable-in-conduit technology, more familiar in the fusion energy community than in high energy physics. The conductor is stabilized by copper, as the temperatures during conductor fabrication comes close to the melting point of aluminum. The conductor jacket is stainless steel, due to the high magnetic stresses. A high-temperature superconducting insert of 6+ T is appealing – but its inner radius would also have to be large to permit shielding against radiation damage. >1000 superconducting wires Incoloy Alloy 908 Conduit Supercritical helium flows in interstices and central channel KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 5

Overview of Radiation Issues for the Solenoid Magnets The magnets at a Muon Collider and Neutrino Factory will be subject to high levels of radiation damage, and high thermal loads due to secondary particles, unless appropriately shielded. To design appropriate shielding it is helpful to have quantitative criteria as to maximum sustainable fluxes of secondary particles in magnet conductors, Si atom and as to the associated thermal load. displaced We survey such criteria first for superconducting magnets, with 50 and then for room-temperature copper magnets. keV A recent review is by H. Weber, Int. J. Mod. Phys. 20 (2011), http://puhep1.princeton.edu/~mcdonald/examples/magnets/weber_ijmpe_20_11.pdf Also, RESMM’12: https://indico.fnal.gov/conferenceDisplay.py?confId=4982 Most relevant radiation-damage data is from “reactor” neutrons (~ 1-10 MeV). Models of radiation damage to materials associate this with “displacement” of the electronic (not nuclear) structure of atoms, with a “defect” being induced by  25-100 eV of deposited energy (although it takes only a few eV to displace an atom from a “lattice,” and defects can be produced by displacement of electrons from atoms without motion of the nucleus). Classic reference: G.H. Kinchin and R.S. Pease, Rep. Prog. Phys. 18 , 1 (1955), http://puhep1.princeton.edu/~mcdonald/examples/magnets/kinchin_rpp_18_1_55.pdf “For displacement effects, a useful parameter is the total amount of energy imparted in displacing collisions.” – V.A.J. van Lint, The Physics of Radiation Damage in Particle Detectors , NIM A253 , 453 (1987), http://puhep1.princeton.edu/~mcdonald/examples/magnets/vanlint_nim_a253_453_87.pdf Hence, it appears to me most straightforward to relate damage limits to (peak) energy deposition in materials. [In our case, u se of DPA = displacements per atom is an unnecessary intermediate step, with no simple relation between DPA and damage , http://www.hep.princeton.edu/~mcdonald/mumu/target/RESMM12/li.pdf ] Reactor-neutron radiation damage is closely equivalent to damage induced by high-energy cascades of the same local energy deposition ( but not to that from, say, an 55 Fe source ). KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 6

Radiation Damage to Superconductor The ITER project quotes the lifetime radiation dose to the superconducting magnets as 10 22 n /m 2 for reactor neutrons with E > 0.1 MeV. This is also 10 7 Gray = 10 4 J/g accumulated energy deposition. For a lifetime of 10 “years” of 10 7 s each, the peak rate of energy deposition would be 10 4 J/g / 10 8 s = 10 -4 W/g = 0.1 mW/g (= 1 MGray/year of 10 7 s). The ITER Design Requirements document, http://puhep1.princeton.edu/~mcdonald/examples/magnets/iter_fdr_DRG1.pdf reports this as 1 mW/cm 3 of peak energy deposition (which seems to imply  magnet  10 g/cm 3 ). Damage to Nb-based superconductors appears to become significant at doses of 2-3  10 22 n /m 2 : A. Nishimura et al ., Fusion Eng. & Design 84 , 1425 (2009) http://puhep1.princeton.edu/~mcdonald/examples/magnets/nishimura_fed_84_1425_09.pdf Reviews of these considerations for ITER: J.H. Schultz, IEEE Symp. Fusion Eng. 423 (2003) http://puhep1.princeton.edu/~mcdonald/examples/magnets/schultz_ieeesfe_423_03.pdf http://puhep1.princeton.edu/~mcdonald/examples/magnets/schultz_cern_032205.pdf Reduction of critical current of various Nb-based Conductors as a function of reactor neutron fluence. From Nishimura et al. KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 7

Radiation Damage to Organic Insulators R&D on reactor neutron damage to organic insulators for conductors is carried out at the Atominstitut, U Vienna, http://www.ati.ac.at/ Recent review: R. Prokopec et al ., Fusion Eng. & Design 85 , 227 (2010) http://puhep1.princeton.edu/~mcdonald/examples/magnets/prokopec_fed_85_227_10.pdf The usual claim seems to be that “ordinary” expoy-based insulators have a useful lifetime of 10 22 n /m 2 for reactor neutrons with E > 0.1 MeV. This is, I believe, the underlying criterion for the ITER limit that we have recently adopted in the Target System Baseline, http://puhep1.princeton.edu/~mcdonald/mumu/target/target_baseline_v3.pdf Efforts towards a more rad hard epoxy insulation seem focused on cyanate ester (CE) resins, which are somewhat expensive (and toxic) . My impression is that use of this insulation brings about a factor of 2 improvement in useful lifetime, but see the cautionary summary of the 2 nd link above. Failure mode is loss of shear strength. Plot show ratio of shear strentgth (ILSS) To nominal for several CE resin variants at reactor neutron fluences of 1-5  10 22 n /m 2 . From Prokopec et al. KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 8

Radiation Damage to the Stabilizer Superconductors for use in high thermal load environments are fabricated as cable in conduit, with a significant amount of copper or aluminum stabilizer (to carry the current temporarily after a quench). The resistivity of Al is 1/3 that of Cu at 4K (if no radiation damage),  Could be favorable to use Al. [Al not compatible with Nb3Sn conductor fabrication  Must use Cu stabilize in high-field Nb magnets.] Radiation damage equivalent to 10 21 n /m 2 doubles the resistivity of Al and increases that of Cu by 10%. http://puhep1.princeton.edu/~mcdonald/examples/magnets/klabunde_jnm_85-86_385_79.pdf Annealing by cycling to room temperature gives essentially complete recovery of the low-temperature resistivity of Al, but only about 80% recovery for copper. Cycling copper-stabilized magnets to room temperature once a year would result in about 20% increase in the resistivity of copper stabilizer in the “hot spot” over 10 years; Al-stabilized magnets would have to be cycled to room temperature several times a year). http://puhep1.princeton.edu/~mcdonald/examples/magnets/guinan_jnm_133_357_85.pdf Hence, Cu stabilizer is preferred if want to operate near the ITER limit (and in high fields). KT McDonald MAP Winter Meeting (SLAC) Mar 5, 2012 9